Fuel cell

ABSTRACT

A fuel cell includes: an electrolyte membrane; first and second catalyst layers respectively formed on first and second surfaces of the electrolyte membrane; and a separator, the first catalyst layer being arranged between the separator and the electrolyte membrane, wherein the separator includes first and second grooves through which reactant gas flows between the first catalyst layer and the separator.

CROSS-REFERENCE TO RELATED APPLICATION

This application is based upon and claims the benefit of priority of theprior Japanese Patent Application No. 2018-155648, filed on Aug. 22,2018, and Japanese Patent Application No. 2018-063276, filed on Mar. 28,2018, the entire contents of which are incorporated herein by reference.

FIELD OF THE INVENTION

The present disclosure relates to a fuel cell.

BACKGROUND

A separator of a fuel cell is formed with grooves through which reactantgas flows between the separator and a catalyst layer formed on anelectrolyte membrane. The reactant gas flowing through the grooves ispartially supplied to the catalyst layer to generate a power generationreaction. For example, grooves of the separator include wavy portionswavily extending, in Japanese Unexamined Patent Application PublicationNo. 2006-147466.

In order to guide the reactant gas from the wavy portions in thedifferent direction within the plane of the separator, it is conceivableto provide a linear portion linearly extending in the differentdirection from the wavy portion in each groove. In a case where suchgrooves are provided, depending on a connection point between the linearportion and the wavy portion, an angle between a tangential direction ofthe wavy portion at the connection point and the linear portion mightdiffer for each of the grooves. Also, the pressure loss of the reactantgas might differ for each of the grooves. Such a difference in pressureloss between the grooves might increase the flow rate of the reactantgas in one of the groove and might decrease the flow rate of thereactant gas in the other groove. Thus, the reactant gas might be hardlysupplied to a part of the catalyst layer, so that the power generationperformance might be deteriorated.

SUMMARY OF THE INVENTION

It is an object of the present disclosure to provide a fuel cell thatsuppresses deterioration of power generation performance.

The above object is achieved by a fuel cell including: an electrolytemembrane; first and second catalyst layers respectively formed on firstand second surfaces of the electrolyte membrane; and a separator, thefirst catalyst layer being arranged between the separator and theelectrolyte membrane, wherein the separator includes first and secondgrooves through which reactant gas flows between the first catalystlayer and the separator, each of the first and second grooves includes:a wavy portion wavily extending in a first direction; a linear portionlinearly extending in a second direction intersecting the firstdirection, and located away from the wavy portion in the firstdirection; and a connecting portion connecting the wavy portion and thelinear portion, the connecting portions of the first and second groovesrespectively include first and second parts, and the first and secondparts linearly extend from the wavy portion to the linear portion inrespective directions that are substantially identical to the firstdirection or are between the first and second directions.

The linear portions of the first and second grooves linearly extend inthe same second direction, and the first and second parts linearlyextend from the wavy portion to the linear portion in respectivedirections that are substantially identical to the first direction orare between the first and second directions. Therefore, in the first andsecond grooves, the angular difference between the wavy portion and theconnecting portion at the connecting point therebetween is small, andthe angular difference between the first part and the linear portion andthe second part and the linear portion is small. This suppresses anincrease in the difference in pressure loss of the reactant gas betweenthe first and second grooves, which suppresses the reactant gas frombeing hardly supplied to a part of the first catalyst layer. Thus, thedeterioration of the power generation performance is suppressed.

An angle between the first part and the wavy portion of the firstgroove, at a connection point between the connecting portion of thefirst groove and the wavy portion of the first groove, may be identicalto an angle between the second part and the wavy portion of the secondgroove, at a connection point between the connecting portion of thesecond groove and the wavy portion of the second groove.

The connecting portion of the first groove may extend in a tangentialdirection of the wavy portion of the first groove at a connection pointbetween the connecting portion of the first groove and the wavy portionof the first groove.

Each length of the connecting portions of the first and second groovesin the first direction may be equal to or smaller than each wavelengthof the wavy portions of the first and second grooves.

The second groove may be adjacent to the first groove, the separator mayinclude a third groove adjacent to the first groove, the first groovemay be arranged between the third and second grooves, the third groovemay include a wavy portion wavily extending in the first direction, thewavy portion of the third groove, the wavy portion of the first groove,and the connecting portion of the second groove may be arranged in adirection orthogonal to the first direction, and amplitude of the wavyportion of the first groove may be smaller than that of the wavy portionof the third groove.

The linear portion of the first groove and the linear portion of thesecond groove may be commonly used.

The first catalyst layer may include an edge extending along the firstdirection, and the part of the connecting portion of the first groovemay extend along the edge.

The first catalyst layer may include: a first edge extending along thefirst direction; and a second edge extending continuously from the firstedge in a direction different from a direction in which the first edgeextends, the connecting portion of the first groove may be locatedbetween the first edge of the first catalyst layer and the connectingportion of the second groove, the linear portion of the first groove maybe located between the second edge of the first catalyst layer and thelinear portion of the second groove, and a connection point between thelinear portion of the first groove and the connecting portion of thefirst groove may be close to the second edge, as compare with aconnection point between the linear portion of the second groove and theconnecting portion of the second groove.

The separator may include first and second manifold holes through whichthe reactant gas flows, the connecting portions of the first and secondgrooves may be close to the first manifold hole, as compared with thesecond manifold hole, and the connecting portions of the first andsecond grooves may be located outside a region that is formed byprojecting the first manifold hole toward the second manifold hole in adirection parallel to the first direction.

The fuel cell may include another separator different from theseparator, the second catalyst layer may be arranged between theelectrolyte membrane and the another separator, the another separatormay include flow path grooves linearly extending, and the connectingportions of the first and second grooves may face the flow path groovesof the another separator via the electrolyte membrane and the first andsecond catalyst layers, and may extend in a direction intersecting theflow path grooves of the another separator.

The wavy portion of at least one of the first and second grooves mayinclude a wavy shape having a constant wavelength and constantamplitude, and extending with a length greater than a length of oneperiod.

The wavy portions of the first and second grooves may have identicalwavelength, identical amplitude, and identical phase, and may beadjacent to each other.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is an exploded perspective view of a unit cell of a fuel cell;

FIG. 2 is a partially cross-sectional view of the fuel cell where theunit cells are stacked;

FIG. 3 is an enlarged view illustrating a part of a flow path portion ofa separator in the present embodiment;

FIG. 4A is an enlarged view illustrating a part of a flow path portionof a separator in a first comparative example, and FIG. 4B is anenlarged view illustrating a part of a flow path portion of a separatorin a second comparative example;

FIG. 5A is an explanatory view of a difference in pressure loss of anodegas in a configuration in which an angle at a connection point between awavy portion and a connecting portion extending in the same directiondiffers for each of grooves, and FIG. 5B is an explanatory view of thedifference in pressure loss of the anode gas in the first comparativeexample;

FIG. 6 is an enlarged view illustrating a part of a flow path portion ofa separator in a first variation;

FIG. 7 is an enlarged view illustrating a part of a flow path portion ofa separator in a second variation;

FIG. 8A is an enlarged view illustrating a part of a flow path portionof a separator in a third variation, and FIG. 8B is an enlarged viewillustrating a part of a flow path portion of a separator in a fourthvariation; and

FIG. 9 is an enlarged view illustrating a part of a flow path portion ofa separator in a fifth variation.

DETAILED DESCRIPTION

FIG. 1 is an exploded perspective view of a unit cell 2 of a fuel cell1. The fuel cell 1 is configured by stacking unit cells 2. FIG. 1illustrates only one unit cell 2, and omits other unit cells. The unitcell 2 is stacked with other unit cells in the Z direction illustratedin FIG. 1. The unit cell 2 has a substantially rectangular shape. Thelongitudinal direction and the short direction of the unit cell 2correspond to the Y direction and the X direction illustrated in FIG. 1,respectively.

The fuel cell 1 is a polymer electrolyte fuel cell that generateselectric power with a fuel gas (for example, hydrogen) and an oxidantgas (for example, oxygen) as reactant gases. The unit cell 2 includes: amembrane electrode gas diffusion layer assembly (MEGA) 10; a supportframe 18 supporting the MEGA 10; a cathode separator 20 and an anodeseparator 40 (hereinafter referred to as separators) sandwiching theMEGA 10. The MEGA 10 has a cathode gas diffusion layer 16 c and an anodegas diffusion layer 16 a (hereinafter referred to as diffusion layers).The support frame 18 has a substantially frame shape, and its innerperipheral side is joined to a peripheral region of the MEGA 10.

Holes c1 to c3 are formed along one of two short sides of the separator20, and holes c4 to c6 are formed along the other side. Likewise, holess1 to s3 are formed along one side of two short sides of the supportframe 18, and holes s4 to s6 are formed along the other side. Likewise,holes a1 to a3 are formed along one side of two short sides of theseparator 40, and holes a4 to a6 are formed along the other side. Theholes c1, s1, and a1 communicate with one another to define a cathodeinlet manifold. Likewise, the holes c2, s2, and a2 define a coolantinlet manifold. The holes c3, s3, and a3 define an anode outletmanifold. The holes c4, s4, and a4 define an anode inlet manifold. Theholes c5, s5, and a5 define a coolant outlet manifold. The holes c6, s6,and a6 define a cathode outlet manifold. In the fuel cell 1 according tothe present embodiment, liquid cooling water is used as a coolant.

A surface of the separator 40 facing the MEGA 10 is formed with an anodeflow path portion 40A (hereinafter referred to as flow path portion)which communicate the anode inlet manifold with the anode outletmanifold and along which the fuel gas flows. The surface of theseparator 20 facing the MEGA 10 is formed with a cathode flow pathportion 20A (hereinafter referred to as flow path portion) whichcommunicate the cathode inlet manifold with the cathode outlet manifoldand along which the oxidant gas flows. The surface of the separator 40opposite to the flow path portion 40A and the surface of the separator20 opposite to the flow path portion 20A are respectively formed withcoolant flow path portions 40B and 20B (hereinafter referred to as flowpath portions) which communicate the coolant inlet manifold with thecoolant outlet manifold and along which the coolant flows. The flow pathportions 20A and 20B extend in the longitudinal direction of theseparator 20 (Y direction). Likewise, the flow path portions 40A and 40Bextend in the longitudinal direction of the separator 40 (Y direction).Each flow path portion is basically provided in a region, facing theMEGA 10, of the separator in the XY plane. The separators 20 and 40 aremade of a material having a gas blocking property and electricalconductivity, and are thin plate shaped members formed by pressingstainless steel, metal such as titanium or titanium alloy. FIG. 1illustrates regions A, B, C, and D on the flow path portion 40A of theseparator 40 that are surrounded by dotted lines, as will be describedlater in detail.

FIG. 2 is a partially cross-sectional view of the fuel cell 1 where theunit cells 2 are stacked. FIG. 2 illustrates only one unit cell 2, andomits the other unit cells. FIG. 2 illustrates a cross sectionorthogonal to the Y direction.

The MEGA 10 includes the diffusion layers 16 a and 16 c, and a membraneelectrode assembly (MEA) 11. The MEA 11 includes an electrolyte membrane12, and an anode catalyst layer 14 a and a cathode catalyst layer 14 c(hereinafter referred to as catalyst layers) formed on one surface andthe other surface of the electrolyte membrane 12, respectively. Theelectrolyte membrane 12 is a solid polymer thin film, such as afluorine-based ion exchange membrane, with high proton conductivity in awet state. The catalyst layers 14 a and 14 c are made by coating acatalyst ink containing a carbon support carrying platinum (Pt) or thelike and an ionomer having proton conductivity on the electrolytemembrane 12. The diffusion layers 16 a and 16 c are made of a materialhaving gas permeability and conductivity, for example, a porous fiberbase material such as carbon fiber or graphite fiber. The diffusionlayers 16 a and 16 c are joined to the catalyst layers 14 a and 14 c,respectively.

Each of the flow path portions 20A, 20B, 40A, and 40B has a wavy shapein cross section when viewed in the Y direction. Specifically, regardingthe flow path portion 20A, a flow path groove 21, recessed away from thediffusion layer 16 c, and a rib 23, protruding to and contacting withthe diffusion layer 16 c, are alternately arranged in the X direction.The cathode gas, flowing along the insides of the flow path grooves 21,is supplied to the catalyst layer 14 c of the MEA 11 via the diffusionlayer 16 c. Further, regarding the flow path portion 20B, a rib 22,protruding opposite to the diffusion layer 16 c and contacting with ananode separator of another unit cell (not illustrated) adjacent to theseparator 20 in the −Z direction, and a flow path groove 24, recededaway from this anode separator, are alternately arranged in the Xdirection. The coolant flows along the insides of the flow path grooves24. Herein, the flow path grooves 21 and the ribs 22 are formedintegrally on the front and rear surfaces, and the ribs 23 and the flowpath grooves 24 are formed integrally on the front and rear surfaces.The flow path grooves 21 and 24 and the ribs 22 and 23 extend in the Ydirection.

Likewise, regarding the flow path portion 40A, a flow path groove 41,recessed away from the diffusion layer 16 a, and a rib 43, protruding toand contacting with the diffusion layer 16 a are alternately arranged inthe X direction. The anode gas, flowing along the insides of the flowpath grooves 41, is supplied to the catalyst layer 14 a of the MEA 11via the diffusion layer 16 a. Further, regarding the flow path portion40B, a rib 42, protruding opposite to the diffusion layer 16 a andcontacting with a cathode separator of another unit cell (notillustrated) adjacent to the separator 40 in the +Z direction, and aflow path groove 44, receded away from this cathode separator, arealternately arranged in the X direction. The coolant flows along theinsides of the flow path grooves 44. Herein, the flow path grooves 41and the ribs 42 are formed integrally on the front and rear surfaces,and the ribs 43 and the flow path grooves 44 are formed integrally onthe front and rear surfaces. The flow path grooves 41 and 44 and theribs 42 and 43 extend in the Y direction.

FIG. 3 is an enlarged view illustrating a part of the flow path portion40A of the separator 40 in the present embodiment. FIG. 3 illustratesthe vicinity of a region A illustrated in FIG. 1. FIG. 3 partiallyillustrates grooves 411 to 415 as a part of the flow path grooves 41.Each of the grooves 411 to 415 includes a wavy portion 41 a, aconnecting portion 41 c, and a linear portion 41 e. These wavy portions41 a wavily extend from the right side of FIG. 3 in the −Y direction.The wavy portions 41 a are substantially the same in a pitch intervalbetween the grooves in the X direction, in wavelength, in phase, and inamplitude. The −Y direction corresponds to the first direction. Eachwavy portion 41 a has a constant wavelength, and a constant amplitude,and a length greater than one period. The connecting portion 41 c islocated in the −Y direction from the wavy portion 41 a and extendstherefrom in the same −Y direction, but has a linear shape differentfrom the shape of the wavy portion 41 a. These connecting portions 41 cextend in substantially the same direction and in substantially parallelto one another. These connecting portions 41 c preferably extendcompletely in the same direction, but for example, they may extendsubstantially in parallel with an angular difference of ±10 degrees orless or ±5 degrees or less. Additionally, these connecting portions 41 cmay extend with an angular difference of ±10 degrees or less or ±5degrees or less with respect to the −Y direction. The linear portion 41e is located away from the wavy portion 41 a in the −Y direction andextends from the connecting portion 41 c in a direction intersecting the−Y direction, specifically, linearly extends in a direction between the−Y direction and the −X direction. The direction in which the linearportion 41 e extends corresponds to the second direction. The linearportion 41 e extends from the connecting portion 41 c toward the holea3. The linear portions 41 e are also substantially parallel to oneanother. As will be described later, FIG. 3 illustrates the wavelength 2of the wavy portion 41 a and the maximum length L of the connectingportion 41 c.

The wavy portions 41 a are formed substantially at the center on the XYplane of the flow path portion 40A. The connecting portions 41 c and thelinear portions 41 e are formed near the end portion located away fromthe center in the −Y direction on the XY plane of the flow path portion40A. A connection point 41 b indicates between the wavy portion 41 a andthe connecting portion 41 c. A connection point 41 d indicates betweenthe connecting portion 41 c and the linear portion 41 e. The connectionpoints 41 b are arranged in the X direction. The connection points 41 dare arranged in a direction intersecting the X direction. Althoughillustration of portions of the wavy portions 41 a on the +Y directionis omitted in FIG. 3, the wavy portions 41 a extend toward the vicinityof the ends, located away from the center in the +Y direction, of theflow path portion 40A. Although illustration is omitted in FIG. 3, theend portion of the linear portions 41 e extend toward the hole a3.Additionally, parts where the linear portions 41 e are not illustratedmay be partially curved before reaching the hole 3 a. Among the flowpath grooves 41 formed in the flow path portion 40A, the groove 411 islocated farthest from the center in the +X direction. Among the linearportions 41 e, the linear portion 41 e of the groove 411 is locatedfarthest from the center in the −Y direction. Additionally, FIG. 3illustrates an edge 14 a 1 of the catalyst layer 14 a located away fromthe center in the +X direction. FIG. 3 illustrates an edge 14 a 2located away from the center in the −Y direction and orthogonal to theedge 14 a 1. The edge 14 a 1 is substantially perpendicular to the Xdirection and extends substantially linearly in the Y direction. Theedge 14 a 2 is substantially perpendicular to the Y direction andextends substantially linearly in the X direction. The edges 14 a 1 and14 a 2 are an example of a first edge and a second edge continuing tothe first edge and extending in a direction different from the directionin which the first edge extends. Among the flow path grooves 41, atleast a part of the grooves 411 to 415 illustrated in FIG. 3 overlap thecatalyst layer 14 a in the Z direction.

Although the ribs 43 illustrated in FIG. 2 are represented withoutnumerical references in FIG. 3, the ribs 43 are formed between adjacentgrooves. The shapes of the ribs 43 also correspond to those of thegrooves 411 to 415. For example, a part of the rib 43 also extendswavily between the wavy portions 41 a. Further, a part of the rib 43also extends linearly between the connecting portions 41 c. Likewise, apart of the rib 43 extends linearly between the linear portions 41 e. Asdescribed above, each of the wavy portions 41 a of the grooves 411 to415 has a constant wavelength and amplitude and extends beyond a lengthof one period. Therefore, a part of the rib 43 also extends wavilybeyond the length of one period, which ensures the flow path grooves 41and the ribs 43 each of which is partially wavily shaped.

Referring to FIG. 2, a description will be given of one of the mainreasons why at least the flow path grooves 41 and the ribs 43 arepartially wavy shaped. For example, in a case where all of the flow pathgrooves 41 and the ribs 43 of the separator 40 and all of the flow pathgrooves 21 and the ribs 23 of the separator 20 are linear, if therelative position between the separators 20 and 40 is displaced from thedesired position in the planar direction, the rib 23 of the separator 20is positionally displaced from the rib 43 of the separator 40 in the Xdirection in the state where the MEGA 10 is sandwiched therebetween.Since the MEGA 10 has low rigidity, if the ribs 23 of the separator 20are positionally displaced from the ribs 43 of the separator 40 in the Xdirection in a long range (for example, 4 mm or more) in the Ydirection, the MEGA 10 might be bent to be locally subjected to strongstress, so that the strength of the MEA 11 might decrease. In contrast,in a case where the flow path grooves 21 and the ribs 23 of theseparator 20, facing the wavy portions 41 a of the flow path grooves 41and the wavy portion of the ribs 43 via the MEGA 10, each has a linearshape, or a wavy shape different from a wavy shape of the wavy portion41 a of the flow path grooves 41 in phase, amplitude, wavelength or thelike, even if the relative position between the separators 20 and 40 isdisplaced from the desired position as described above, the MEGA 10 issuppressed from being bent by positionally displacing the ribs 23 of theseparator 20 from the ribs 43 of the separator 40 in the X direction ina long range in the Y direction. This suppresses the decrease instrength of the MEA 11. In the present embodiment, the flow path grooves21 and the ribs 23 of the separator 20, facing the wavy portions 41 a ofthe flow path grooves 41 and the ribs via the MEGA 10, each has a linearshape, but they not limited thereto.

Next, the present embodiment will be described in comparison withcomparative examples. FIG. 4A is an enlarged view illustrating a part ofa flow path portion 40Ax of a separator 40 x in the first comparativeexample. FIG. 4A corresponds to FIG. 3. Unlike the flow path portion 40Ain the present embodiment, the connecting portions 41 c are notrespectively provided in the flow path portion 40Ax of the separator 40x, and wavy portions 41 ax of grooves 411 x to 415 x are respectivelyconnected directly to linear portions 41 ex. Herein, connection points41 dx between the wavy portions 41 ax and the linear portions 41 ex arearranged in a direction intersecting the X direction, like the directionin which the connection points 41 d are arranged in the presentembodiment. Herein, the wavy portions 41 ax are substantially the samein phase and wavelength. Therefore, the phase position of the wavyportion 41 ax at the connection point 41 dx differs for each of thegrooves 411 x to 415 x, and the tangential direction of the wavy portion41 ax at the connection point 41 dx also differs for each of the grooves411 x to 415 x. Thus, the angle between the tangential direction of thewavy portion 41 ax at the connection point 41 dx and the extendingdirection of the linear portion 41 ex also differs for each of thegrooves 411 x to 415 x. Accordingly, the pressure loss of the anode gasas well as the flow rate of the anode gas differ for each of the grooves411 x to 415 x. For example, the groove 415 x at the connection point 41dx continues from the wavy portion 41 ax to the linear portion 41 ex atan acute angle. However, the groove 411 x at the connection point 41 dxgently continues from the wavy portion 41 ax to the linear portion 41ex, as compared with the groove 415 x. The pressure loss of the anodegas might be larger in the groove 415 x than in the groove 411 x, andthe flow rate of the anode gas might be smaller in the groove 415 x thanin the groove 411 x. In this way, the difference in flow rate of theanode gas between the grooves 411 x to 415 x might increase, and theanode gas might be hardly supplied to a part of the catalyst layer 14 a.As a result, the power generation performance might be deteriorated.

On the other hand, in the present embodiment illustrated in FIG. 3, thewavy portion 41 a is not directly connected to the linear portion 41 e,but via the connecting portion 41 c linearly extending. Therefore, theangle between the connecting portion 41 c and the linear portion 41 e atthe connection point 41 d is substantially the same for each of thegrooves 411 to 415. This suppresses the increase in the difference inpressure loss of the anode gas between the grooves 411 to 415, andsuppresses the increase in the difference in flow rate of the anode gastherebetween. This also suppresses the anode gas from being hardlysupplied to a part of the catalyst layer 14 a. This also suppresses thedeterioration of the power generation performance due to deteriorationof the catalyst layer 14 a caused by hydrogen deficiency.

Further, in the present embodiment, the phase position of the wavyportion 41 a at the connection point 41 b is substantially the same foreach of the grooves 411 to 415. Therefore, the angle between thetangential direction of the wavy portion 41 a and the extendingdirection of the connecting portion 41 c at the connection point 41 b issubstantially the same for each of the grooves 411 to 415. Thissuppresses the increase in the difference in pressure loss of the anodegas between the grooves 411 to 415, and suppresses the increase in thedifference in flow rate of the anode gas therebetween. This alsosuppresses the deterioration of the power generation performance.

Furthermore, in the present embodiment, the connecting portion 41 cextends in the tangential direction of the wavy portion 41 a at theconnection point 41 b. Therefore, the wavy portion 41 a smoothlycontinues to the connecting portion 41 c at the connection point 41 b,which suppresses the increase in pressure loss of the anode gas. Thisconfiguration ensures each flow rate of the anode gas flowing throughthe grooves 411 to 415, and the anode gas is supplied to the entirecatalyst layer 14 a.

FIG. 4B is an enlarged view illustrating a part of a flow path portion40Ay of a separator 40 y in a second comparative example. FIG. 4Bcorresponds to FIG. 3. Unlike the flow path portion 40A in the presentembodiment, the angle between the extending direction of a linearportion 41 ey and the Y direction is smaller than that between theextending direction of the linear portion 41 e and the Y direction inthe present embodiment. Connection points 41 dy between wavy portions 41ay and the linear portions 41 ey are arranged in the X direction. Thewavy portions 41 ay have substantially the same phase and wavelength.Therefore, the phase position of the wavy portion 41 ay at theconnection point 41 dy is substantially the same for each of grooves 411y to 415 y, and the flow rate of the anode gas is also substantially thesame for each of the grooves 411 y to 415 y. However, as illustrated inFIG. 4B, the grooves 411 y to 415 y not extend to the vicinity of acorner portion X of the catalyst layer 14 a between the edge 14 a 1 andthe edge 14 a 2. Therefore, the anode gas might not be sufficientlysupplied to the corner portion X, which might degrade the powergeneration performance.

On the other hand, in the present embodiment illustrated in FIG. 3, eachof the grooves 411 to 415 includes the connecting portion 41 c extendingfrom the wavy portion 41 a to the edge 14 a 2 of the catalyst layer 14a, and the connection point 41 d of the groove 411 that is the closestto the edge 14 a 1 is the closest to the edge 14 a 2. Specifically, thegrooves 411 to 415 are arranged in ascending order of the distancebetween the connection point 41 d and the edge 14 a 2. In other words,the connecting portion 41 c of the groove 411 closest to the edge 14 a 1among the connecting portions 41 c is the longest, under the conditionthat the connection points 41 b of the grooves 411 to 415 aresubstantially the same in position in the Y direction. In this way, thegroove 411 extends to the vicinity of the corner portion of the catalystlayer 14 a, and a part of the anode gas flowing through the groove 411is supplied to the corner portion of the catalyst layer 14 a. Thissuppresses the anode gas from being hardly supplied to a part of thecatalyst layer 14 a, which suppresses the deterioration of the powergeneration performance.

In the present embodiment, a length of the connecting portion 41 c ofthe groove 411 is the maximum length L of the connecting portions 41 cin the Y direction, but the maximum length L is less than or equal tothe wavelength λ of the wavy portion 41 a. That is, each connectingportion 41 c is shorter than the wavelength λ of the wavy portion 41 ain the Y direction. The present embodiment ensures the ratio of the areaof the wavy portions 41 a to the area of the flow path portion 40A inthe XY plane. Such a configuration suppresses the MEGA 10 from beingbent over a long range in the Y direction as described above, whichsuppresses the decrease in strength of the MEA 11.

Next, the region A illustrated in FIG. 1 will be described. The region Ais an area where at least the connecting portions 41 c are formed.Additionally, FIG. 1 illustrates a region C formed by projecting thehole a3 toward the hole a4 in the +Y direction. The region A is locatedcloser to the hole a3 than the hole a4 and away from the region C in the+X direction. Preferably, the connecting portions 41 c are formed insuch a region A. The reason is as follows. Although the hole a3 islocated at an end of the separator 40 that is located away from thecenter in the −X direction, the region A is located on the side of theseparator 40 away from the center in the +X direction. Accordingly, itis needed to guide the anode gas flowing on the side, of the flow pathportion 40A of the separator 40, located away from the center in the +Xdirection, to the hole a3. The above description does not mean theconnecting portions 41 c are limited to be formed in the region A in thepresent embodiment. The connecting portions 41 c may be formed outsidethe region A.

Preferably, grooves including the connecting portions illustrated inFIG. 3 are also formed in a region B. The regions A and B aresymmetrical with respect to the center on the XY plane of the flow pathportion 40A. Preferably, the shape of the grooves formed in the region Band the shape of the grooves 411 to 415 illustrated in FIG. 3 aresymmetrical with respect to the center on the XY plane of the flow pathportion 40A. Additionally, FIG. 1 illustrates a region D formed byprojecting the hole a4 toward the hole a3 in the −Y direction.Preferably, the region B is located closer to the hole a4 than the holea3 and away from the region D in the −X direction. This is because it isneeded to guide a part of the anode gas, flowing from the hole a4 to thehole a3 via the flow path portion 40A, toward the end of the flow pathportion 40A away from the other ends in the −X direction. The abovedescription does not mean the connecting portions 41 c are limited to beformed in the region B in the present embodiment. The connectingportions 41 c may be formed outside the region B. The holes a3 and a4are examples of the first and second manifold holes through which theanode gas flows.

The wavy portions 41 a of the grooves 411 to 415 have substantially thesame wavelength, the same phase, the same amplitude, and the commonshape. Here, in general, as for pressing, the shape of a metal plateformed by dies is not always the same as the reversed shape of the die.After the metal plate is deformed by the die, the shape of the metalplate slightly becomes to its original shape before the molding, due tothe elasticity of the metal plate. This is called spring back. For thisreason, this spring back is taken into consideration in designing thedies. In a case where groove shapes differ from each other, it might beneeded to design the dies for the respective groove shapes, and it mighttake long time for designing the die. In the present embodiment, thegrooves have the common shape. It is thus possible to suppress the longtime required to design the dies. In the case of forming a precise shapelike a separator for a fuel cell, the metal plate is pressed withdifferent dies several times, so that the metal plate is graduallyexpanded to achieve the final product shape. In a case where the wavyshapes in the final product shape differ from each other, the design ofthe dies used in pressing is different, so that the time required todesign the dies might be further prolonged. On the other hand, the wavyportions 41 a of the grooves 411 to 415 have the common shape in thepresent embodiment. It is thus possible to form the common shape in thedies for pressing, and to suppress the prolongation of the time requiredto design the dies for producing the separator.

In the present embodiment, as illustrated in FIG. 3, the phase of thewavy portion 41 a at the connection point 41 b is the same for each ofthe grooves 411 to 415. In other words, the angle between the wavyportion 41 a and the connecting portion 41 c at the connection point 41b is the same for each of the grooves 411 to 415. However, even in acase where the angle between the wavy portion 41 a and the connectingportion 41 c at the connection point 41 b differs for each of thegrooves 411 to 415, it is possible to suppress the increase in thedifference in pressure loss of the anode gas as compared with the firstcomparative example, as long as the direction in which the connectingportion 41 c extends is substantially the same as the −Y direction inwhich the wavy portion 41 a extends, that is, as the above-describedfirst direction. This point will be described below.

FIG. 5A is an explanatory view of a difference in pressure loss of theanode gas in a configuration in which an angle at a connection pointbetween a wavy portion and a connecting portion extending in the samedirection differs for each of grooves. FIG. 5A illustrates the groove411 having a curved shape, points P1 to P4 on the groove 411, tangentialdirections a1 to a4 of the groove 411 at the points P1 to P4, and thedirections A on the points P1 to P4. The points P1 to P4 indicate theconnection point between the wavy portion and the connecting portion. Inthe present embodiment, the direction A is the direction in which theconnecting portion extends, and also the direction in which the wavyportion 41 a extends.

For example, in a case where the wavy portion and the connecting portionare connected at the point P1, the anode gas tries to flow to the pointP1 along the wavy portion in the tangential direction a1 and tries toflow from the point P1 along the connecting portion in the direction A.Likewise, in a case where the wavy portion and the connecting portionare connected at the point P2, the anode gas tries to flow to the pointP2 in the tangential direction a2 and tries to flow from the point P2 inthe direction A. In a case where the wavy portion and the connectingportion are connected at the point P3, the anode gas tries to flow tothe point P3 in the tangential direction a3 and tries to flow from thepoint P3 in the direction A. In a case where the wavy portion and theconnecting portion are connected at the point P4, the anode gas tries toflow to the point P4 in the tangential direction a4 and tries to flowfrom the point P4 in the direction A.

Herein, the tangential direction a1 and the direction A at the point P1are the same. Likewise, the tangential direction a3 and the direction Aat the point P3 are the same. Therefore, the angle between thetangential direction a1 and the direction A and the angle between thetangential direction a3 and the direction A are both zero. This angle ateach of the points P1 and P3 is the minimum value of a possible anglebetween the tangential direction of the groove 411 and the direction A,in a case where the wavy portion and the connecting portion areconnected at an arbitrary point on the groove 411. Therefore, forexample, in a case where the wavy portion and the connecting portion areconnected at the point P1, the pressure loss of the anode gas at thepoint P1 is small, since the angle between the tangential direction a1and the direction A is zero. Likewise, in a case where the wavy portionand the connecting portion are connected at the point P3, the pressureloss of the anode gas at the point P3 is small, since the angle betweenthe tangential direction a3 and the direction A is zero.

On the other hand, the angle between the tangential direction a2 and thedirection A is represented by a, and the angle between the tangentialdirection a4 and the direction A is represented by the same a. Herein,the angle α at each of the points P2 and P4 is the maximum value of apossible angle between the tangential direction of the groove 411 andthe direction A, in a case where the wavy portion and the connectingportion are connected at an arbitrary point on the groove 411.Therefore, in a case where the wavy portion and the connecting portionare connected at the point P2, the pressure loss of the anode gas at thepoint P2 is large, since the angle between the tangential direction a2and the direction A is the maximum a. Likewise, in a case where the wavyportion and the connecting portion are connected at the point P4, thepressure loss of the anode gas at the point P4 is large, since the anglebetween the tangential direction a4 at the point P4 and the direction Ais the maximum a. As described above, in a case of providing a groove,in which the wavy portion and the connecting portion are connected atthe point P1 or P3, and a groove, in which the wavy portion and theconnecting portion are connected at the point P2 or P4, the differencein pressure loss of the anode gas between the two grooves is thelargest. The difference between the angle zero at the point P1 or P3 andthe angle α at the point P2 or P4 is α. This difference α correlateswith the magnitude of the difference in pressure loss of the anode gasbetween the two grooves.

FIG. 5B is an explanatory view of the difference in pressure loss of theanode gas in the first comparative example. Like FIG. 5A, FIG. 5Billustrates schematically the groove 411 x, the points P1 to P4, thetangential directions a1 to a4, directions B at the points P1 to P4.Note that the groove 411 illustrated in FIG. 5A and the groove 411 xillustrated in FIG. 5B have the same shape, but the different numericalreferences are given for convenience. The direction B is the directionin which the linear portion 41 ex in the first comparative exampleextends, that is, the above-described second direction. The direction Bgreatly intersects the direction in which the groove 411 x extends. Anangle between the direction B and the −Y direction in which the groove411 x extends is β. β is greater than a.

For example, in a case where the wavy portion 41 ax and the linearportion 41 ex are connected at the point P1, the anode gas tries to flowto the point P1 along the wavy portion 41 ax in the tangential directiona1 and tries to flow from the point P1 along the linear portion 41 ex inthe direction B. Likewise, in a case where the wavy portion 41 ax andthe linear portion 41 ex are connected at the point P2, the anode gastries to flow to the point P2 in the tangential direction a2 and triesto flow from the point P2 in the direction B. In a case where the wavyportion 41 a and the linear portion 41 ex are connected at the point P3,the anode gas tries to flow to the point P3 in the tangential directiona3 and tries to flow from the point P3 in the direction B. In a casewhere the wavy portion 41 a and the linear portion 41 ex are connectedat the point P4, the anode gas tries to flow to the point P4 in thetangential direction a4 and tries to flow from the point P4 in thedirection B.

Herein, the angle between the tangential direction a1 and the directionB at the point P1 and the angle between the tangential direction a3 andthe direction B at the point P3 are both β. The angle between thetangential direction a2 and the direction B at the point P2 is (α+β).Herein, the angle (α+β) at the point P2 is the maximum value of apossible angle between the tangential direction of the groove 411 x andthe direction B, in a case where the wavy portion 41 a and the linearportion 41 ex are connected at an arbitrary point on the groove 411 x.Therefore, the pressure loss of the anode gas at the point P2 is large.The angle between the tangential direction a4 and the direction B at thepoint P4 is (β−α). Herein, the angle (β−α) at the point P4 is theminimum value of a possible angle between the tangential direction ofthe groove 411 x and the direction B, in a case where the wavy portion41 a and the linear portion 41 ex are connected at an arbitrary point onthe groove 411 x. Therefore, the pressure loss of the anode gas at thepoint P4 is small. Herein, in a case of providing a groove, in which thewavy portion 41 a and the linear portion 41 ex are connected at thepoint P2, and a groove, in which the wavy portion 41 a and the linearportion 41 ex are connected at the point P4, the difference in pressureloss of the anode gas between the two grooves is the largest. Thedifference between the angle (α+β) at the point P2 and the angle (β−α)at the point P4 is 2α, and this difference 2α correlates with themagnitude of the difference in pressure loss of the anode gas betweenthe two grooves.

The difference α in the configuration described with reference to FIG.5A is smaller than the difference 2α in the first comparative example.This means that the difference in pressure loss of the anode gas betweenthe grooves in the above configuration is smaller than that in thecomparative example, and that the increase in the difference in flowrate of the anode gas between the grooves is also suppressed in theabove configuration. Therefore, the angle between the wavy portion 41 aand the connecting portion 41 c at the connection point 41 b is the samefor each of the grooves 411 to 415 in the present embodiment, but it isnot limited to this.

The above describes the case where β is greater than a, but it is notlimited to this. In a case where β is smaller than a, the minimum valueof the angle at the connection point is zero unlike the abovedescription, but the maximum value is (α+β) like the above description.Therefore, the maximum value of the possible angle difference is (α+β).The maximum value of the angle difference is α, which is smaller than(α+β), in the case where the direction A of the connecting portion isthe above-described first direction. It is therefore possible tosuppress the increase in difference in pressure loss correlating with anangle difference. Further, the above describes the case where thedirection A of the connecting portion is the first direction, but it isnot limited thereto. Even in a case where the direction of theconnecting portion is between the first direction and the seconddirection, the maximum value of a possible angle is small as comparedwith the case where the wavy portion is connected with the linearportion extending in the second direction. It is therefore possible tosuppress the increase in the difference in pressure loss correlatingwith the angle difference.

Next, variations will be described. In the following variations, thesame reference numerals are given to the same components as those of theabove-described embodiment, and duplicated explanations are omitted.

FIG. 6 is an enlarged view illustrating a part of a flow path portion40Aa of a separator 40 a in a first variation. FIG. 6 corresponds toFIG. 3. The flow path portion 40Aa is formed with grooves 416 to 419 inaddition to the above-described grooves 411 to 415. Like each of thegrooves 411 to 415, each of the grooves 416 to 419 also includes thewavy portion 41 a, the connecting portion 41 c, and the linear portion41 e. The wavy portion 41 a of the groove 416 is adjacent to the wavyportion 41 a of the groove 415 in the −X direction, and the connectingportion 41 c of the groove 416 is shorter than the connecting portion 41c of the groove 415. The connecting portion 41 c of the groove 417 isadjacent to the wavy portion 41 a of the groove 416 in the −X direction,and the connecting portions 41 c of the grooves 417 to 419 are arrangedin the X direction. The connection points 41 d of the grooves 411 to 419are arranged to intersect the X direction. Regarding the grooves 417 to419, the angle between the connecting portion 41 c and the linearportion 41 e at the connection point 41 d is also set to besubstantially the same. The angle between the connecting portion 41 cand the linear portion 41 e at the connection point 41 d in each of thegrooves 417 to 419 is substantially the same as the angle between theconnecting portion 41 c and the linear portion 41 e at the connectionpoint 41 d in each of the grooves 411 to 416. Like the above-describedembodiment, each connecting portion 41 c of the grooves 411 to 419 isconnected to the wavy portion 41 a at the connection point 41 b in thetangential direction of the wavy portion 41 a. Also in the firstvariation, this suppresses the increase in the difference in pressureloss of the anode gas between the grooves 411 to 419, and suppresses thedeterioration of the power generation performance.

FIG. 7 is an enlarged view illustrating a part of a flow path portion40Ab of a separator 40 b in a second variation. A groove 416 b includesthe wavy portion 41 a and a wavy portion 41 ab that extends in the −Ydirection from the wavy portion 41 a and has an amplitude smaller thanthat of the wavy portion 41 a. The wavy portion 41 ab of the groove 416b is adjacent to the wavy portion 41 a of the groove 415 in the +Xdirection, and is adjacent to the linear connecting portion 41 c of thegroove 417 in the −X direction. For example, in a case where theamplitude of the wavy portion 41 ab of the groove 416 b is the same asthat of the wavy portion 41 a, an interval in the X direction betweenthe wavy portion 41 ab and the connecting portion 41 c, having a linearshape of the groove 417 and adjacent to the wavy portion 41 ab in the −Xdirection, partially increases. In this case, the anode gas might behardly supplied to such a part where the interval between the adjacentgrooves partially increases, which might degrade the power generatingperformance. On the other hand, in the second variation, since theamplitude of the wavy portion 41 ab is smaller than that of the wavyportion 41 a of the groove 415 adjacent to the wavy portion 41 ab in the+X direction. This suppresses the increase in the interval between thewavy portions 41 ab and 41 a in the X direction. This also suppressesthe anode gas from being hardly supplied to a part of the catalyst layer14 a, which suppresses the deterioration of the power generationperformance.

In the second variation, when the connecting portion 41 c of the groove417 is interpreted to have a wavy shape with zero amplitude, theamplitude gradually changes in the order of the connecting portion 41 cof the groove 417, the wavy portion 41 ab of the groove 416, and thewavy portion 41 a of the groove 415 that are arranged in the Xdirection. It is therefore possible to suppress an increase in theelongation percentage of the base material in this region, and tosuppress a decrease in the yield rate. It is also possible to reduce theresidual stress in pressing this region. Accordingly, it is possible toreduce the possibility of a warp in the separator 40 b.

In this variation, the grooves 416 b and 417 are examples of the firstand second grooves, respectively. The groove 415 is an example of athird groove. The groove 416 b is arranged between the groove 415 andthe groove 417.

FIG. 8A is an enlarged view illustrating a part of a flow path portion40Ac of a separator 40 c in a third variation. FIG. 8A corresponds toFIG. 3. In the flow path portion 40Ac, grooves 411 c and 412 c share alinear portion 41 ec. Likewise, grooves 413 c to 415 c share the linearportion 41 ec. Specifically, a connecting portion 41 cc of the groove412 c is connected to a part of the linear portion 41 ec of the groove411 c. Likewise, connecting portions 41 cc of the grooves 414 c and 415c are connected to a part of the linear portion 41 ec of the groove 413c. Even in such a configuration, since the connecting portions 41 cclinearly extend in the same direction and the linear portions 41 eclinearly extend in the direction different from the direction of theconnecting portions 41 cc, the angle between the connecting portion 41cc and the linear portion 41 ec is substantially the same for each ofthe grooves 411 c to 415 c. In each of the grooves 411 c to 415 c, theconnecting portion 41 cc is connected to the wavy portion 41 a at theconnection point 41 b in the tangential direction of the wavy portion 41a. This suppresses the increase in the difference in pressure loss ofthe anode gas between the grooves 411 c and 412 c, and also suppressesthe increase in the difference in pressure loss of the anode gas betweenthe grooves 413 c to 415 c, which suppresses the deterioration of thepower generation performance. Additionally, the two grooves 411 c and412 c join each other, and the three grooves 413 c to 415 c join oneanother. It is thus desirable to suppress the increase in the differencebetween the pressure loss of the anode gas in each of the grooves 411 cand 412 c and the pressure loss of the anode gas in each of the grooves413 c to 415 c. For example, a groove cross-sectional area of the linearportion 41 ec of the grooves 413 c to 415 c may be made to be largerthan a groove cross-sectional area of the linear portion 41 ec of thegrooves 411 c and 412 c, which may suppress the increase in thedifference in pressure loss.

Further, the connecting portion 41 cc of the groove 412 c is longer thanthe connecting portion 41 cc of the groove 411 c. The connecting portion41 cc of the groove 414 c is longer than the connecting portion 41 cc ofthe groove 413 c. The connecting portion 41 cc of the groove 415 c islonger than the connecting portion 41 cc of the groove 414 c.Furthermore, connection points 41 dc of the grooves 411 c and 412 c arearranged in such a direction that the linear portion 41 ec shared by thegrooves 411 c and 412 c extends. Likewise, the connection points 41 dcof the grooves 413 c to 415 c are arranged in such a direction that thelinear portion 41 ec shared by the grooves 413 c to 415 c extends.Moreover, the connection point 41 dc of each of the grooves 411 c and412 c and the connection point 41 dc of each of the grooves 413 c to 415c are not located on the same straight line, unlike the above-describedembodiment and the like.

The interval between the adjacent linear portions 41 ec is wider thanthe interval between the adjacent connecting portions 41 cc, and iswider than the interval between the adjacent wavy portions 41 a, but isnot limited thereto. For example, the interval between the adjacentlinear portions 41 ec may be smaller than the interval between theadjacent connecting portions 41 cc, or the interval between the adjacentwavy portions 41 a.

FIG. 8B is an enlarged view illustrating a part of a flow path portion40Ad of a separator 40 d in a fourth variation. Grooves 411 d to 415 din the fourth variation have substantially the same shape as the grooves411 to 415 in the above-described embodiment, and are formed in theregion A. Further, in FIG. 8B, the linearly-extending flow path grooves21 of the separator 20 are illustrated by dotted lines. The connectingportions 41 c of the grooves 411 d to 415 d face the flow path grooves21 via the MEGA 10 and extend in the direction intersecting the flowpath groove 21. That is, the connecting portion 41 c is not parallel tothe flow path groove 21. This suppresses the MEGA 10 from being bentover a long range in the Y direction, thereby suppressing the decreasein the strength of the MEA 11. Since the linear portion 41 e also facesthe flow path groove 21 via the MEGA 10 and extends in the directionintersecting the flow path groove 21, the decrease in the strength ofthe MEA 11 is suppressed. The separator 20 is disposed opposite to theelectrolyte membrane 12 with respect to the catalyst layer 14 c, and isan example of another separator different from the separator 40.

In the case where unit cells are stacked such that the grooves 411 d to415 d of the anode flow path portion 40Ad intersect the cathode flowpath groove 21 in the fourth variation illustrated in FIG. 8B, thecooling water flows between the adjacent unit cells, specifically,between the flow path portion 40B, formed on the rear surface of theflow path portion 40Ad, and the flow path portion 20B, formed on therear surface of the cathode flow path portion 20A. Therefore, inaccordance with the flow path portions 40B and 20B, the cooling watermeanders in the Z direction and flows along the respective flow pathportions in the direction of the XY plane. The flow path through whichthe coolant flows meanders in the Z direction in such a case, thepressure loss of the cooling water may increase. However, by increasingthe groove width of the cooling water, it is possible to suppress theincrease in the pressure loss of the cooling water. That is, in thefourth variation, the interval between the adjacent cathode flow pathgrooves 21, partially intersecting the grooves 411 d to 415 d of theanode flow path portion 40Ad, may be set to be larger than the intervalbetween the adjacent cathode flow path grooves 21, partially notintersecting the grooves 411 d to 415 d of the anode flow path portion40Ad. Further, the interval between the adjacent grooves 411 d to 415 dof the anode flow path portion 40Ad, partially intersecting the cathodeflow path grooves 21, may be set larger than the interval between theadjacent grooves 411 d to 415 d of the anode flow path portion 40Ad,partially not intersecting the cathode flow path grooves 21.

FIG. 9 is an enlarged view illustrating a part of a flow path portion40Ae of a separator 40 e in a fifth variation. In the flow path portion40Ae, unlike the direction in which the wavy portion 41 ae extends, theconnecting portion 41 ce extends from a wavy portion 41 ae to a linearportion 41 ee in the direction between the −Y direction and thedirection in which the linear portion 41 ee extends. Further, theconnecting portion 41 ce extends in the tangential direction of the wavyportion 41 ae at a connection point 41 be between the wavy portion 41 aeand the connecting portion 41 ce. Even in such a configuration, theangle between the connecting portion 41 ce and the linear portion 41 eeat a connection point 41 de is substantially the same for each ofgrooves 411 e to 415 e. This suppresses the increase in the differencein pressure loss of the anode gas between the grooves 411 e to 415 e,and suppresses the deterioration of the power generation performanceAdditionally, the phase position of the wavy portion 41 ae at theconnection point 41 be is substantially the same for each of the grooves411 e to 415 e, which also suppresses the deterioration of the powergeneration performance. Each of the interval between the adjacent linearportions 41 ee and the interval between adjacent connecting portions 41ce is smaller than the interval between adjacent wavy portions 41 ae,but they are not limited thereto.

In the above-described embodiments and variations, the grooves aresubstantially the same in wavelength and phase, but they are not limitedthereto. This is because, as long as the angle between the linearportion and the connecting portion is substantially the same for each ofthe grooves, the increase in the difference in flow rate of the reactantgas between the grooves is suppressed, and the reactant gas issuppressed from being hardly supplied to a part of the catalytic layer.Further, in the above-described embodiment and the variations, thegrooves are formed at substantially the same pitch intervals, but theyare not limited thereto.

The flow path grooves in the present embodiment and variations describedabove may be applied to the cathode separator.

Although the separators 40 to 40 e are adopted in the water-cooled fuelcell 1 using liquid as the coolant, they are not limited thereto, andmay be adopted in an air-cooled fuel cell using air as the coolant.

The wavy groove described above may have a sine wave shape, or a wavyshape with a straight line and an arc.

The wavy portion and the connecting portion may be connected via anarcuate portion having an arcuate shape. In a case where the connectingportion is connected to the wavy portion at the connection pointtherebetween with a bending angle and is not connected to the wavyportion in the tangential direction thereof, the connection between thewavy portion and the connecting portion via the arcuate portionsuppresses the increase in the pressure loss. The arc of the arcuateportion provided in each groove may be the same size or a differentsize. In a case where the arc have the same size, it is possible touniform the pressure loss at the arcuate portion, thereby furthersuppressing the increase in the difference in pressure loss between thegrooves. Likewise, the connecting portion and the linear portion may beconnected via an arcuate portion. The connecting portion is not limitedto a complete linear shape over the entire extended area, and may becurved, for example, in the vicinity of the connection point between theconnecting portion and the wavy portion or the connection point betweenthe connecting portion and the linear portion.

Although some embodiments of the present disclosure have been describedin detail, the present disclosure is not limited to the specificembodiments but may be varied or changed within the scope of the presentdisclosure as claimed.

1. A fuel cell comprising: an electrolyte membrane; first and second catalyst layers respectively formed on first and second surfaces of the electrolyte membrane; and a separator, the first catalyst layer being arranged between the separator and the electrolyte membrane, wherein the separator includes first and second grooves through which reactant gas flows between the first catalyst layer and the separator, each of the first and second grooves includes: a wavy portion wavily extending in a first direction; a linear portion linearly extending in a second direction intersecting the first direction, and located away from the wavy portion in the first direction; and a connecting portion connecting the wavy portion and the linear portion, the connecting portions of the first and second grooves respectively include first and second parts, and the first and second parts linearly extend from the wavy portion to the linear portion in respective directions that are substantially identical to the first direction or are between the first and second directions.
 2. The fuel cell of claim 1, wherein an angle between the first part and the wavy portion of the first groove, at a connection point between the connecting portion of the first groove and the wavy portion of the first groove, is identical to an angle between the second part and the wavy portion of the second groove, at a connection point between the connecting portion of the second groove and the wavy portion of the second groove.
 3. The fuel cell of claim 1, wherein the connecting portion of the first groove extends in a tangential direction of the wavy portion of the first groove at a connection point between the connecting portion of the first groove and the wavy portion of the first groove. 4-5. (canceled)
 6. The fuel cell of claim 1, wherein the linear portion of the first groove and the linear portion of the second groove are commonly used. 7-10. (canceled)
 11. The fuel cell of claim 1, wherein the wavy portion of at least one of the first and second grooves includes a wavy shape having a constant wavelength and constant amplitude, and extending with a length greater than a length of one period.
 12. The fuel cell of claim 1, wherein the wavy portions of the first and second grooves have identical wavelength, identical amplitude, and identical phase, and are adjacent to each other. 